So next, I would like to describe the action of the Steenrod squares in a more general context (which is pure homological algebra). This more general approach to Steenrod operations seems to be due to Peter May, but I learned it from these lecture notes by Jacob Lurie.
As I said earlier, the Steenrod squares will act on the cohomology of any -algebra. What is an
-algebra? It’s supposed to be a dga with a multiplication law that is coherent and associative up to coherent homotopy. Or, equivalently, an algebra over an
-operad in chain complexes. Unfortunately, I don’t know too many simple ones. For instance, the standard
-operad in spaces, the infinite little cubes operad, is huge: the individual terms have to be contractible spaces large enough to admit a free action of the symmetric group.
But we’ll need less structure than an -algebra structure. We’ll need a multiplication law on a chain complex
which is commutative up to coherent homotopy, but without quite all the coherence that one would need for an
-algebra.
What should this be? Well, a multiplication law would be a map , and to say that it is commutative would be to say that it is
-equivariant where
acts by permutation on
and trivially on
. In other words, it would be a map
where
denotes the coinvariants. This is generally going to be too strong: most of the homotopy commutative multiplication laws we deal with will not be rectifiable to strictly commutative ones.
Instead, we’ll use maps not out of the coinvariants of , but out of the homotopy coinvariants. To get this, one first tensors
with a complex of free
-modules which is contractible as a complex of vector spaces, and then takes the coinvariants.
More generally:
Definition 1 If
is a
-equivariant complex of
-vector spaces, then we define the homotopy coinvariants
as the coinvariants of
. Here
is any acyclic resolution of the complex
(just
in degree zero, nothing elsewhere) consisting of free
-modules.